docker_image_falling_fluid_film

All the instructions below are for Linux (typically, a modern Ubuntu). If you are on windows, you will have to adapt the instructions by yourself.

What is contained in this repository?

This repository contains the docker container of the paper Exploiting locality and physical invariants to design effective Deep Reinforcement Learning control of the unstable falling liquid film, Belus et. al., published at https://aip.scitation.org/doi/10.1063/1.5132378 .

If you find this work useful and / or use it in your own research, please cite our works:

V. Belus, J. Rabault, J. Viquerat, Z. Che, E. Hachem, and U. Reglade
Exploiting locality and physical invariants to design effective Deep
Reinforcement Learning control of the unstable falling liquid film,
ArXiv (2019)

This is mostly a mirror of the initial repos at https://github.com/vbelus/falling-liquid-film-drl and https://github.com/vbelus/drl-fluid-film-notebook , with in addition the container image being loaded on the repo using git-lfs.

Getting the container image

The docker image for the falling fluid film repo https://github.com/vbelus/falling-liquid-film-drl and the jupyter notebooks https://github.com/vbelus/drl-fluid-film-notebook , stored with git-lfs. The container has all the content of the corresponding repos already built in, and should be fully ready to use.

The container image is available in the container folder. It is split in segments of max size 500M and committed with git-lfs (in theory git-lfs could commit the whole container, but I encountered issues with large files even in git-lfs in the past, see discussion at A note here in the readme at https://github.com/jerabaul29/Cylinder2DFlowControlDRLParallel).

To download the segments, either clone the repository, or if this fails or times out, download each of the segment "by hand" (click on each file in https://github.com/jerabaul29/docker_image_falling_fluid_film/tree/main/container and use the "download" button).

Splitting the container image was performed with:

$ split -b 500M falling-fluid-film-drl-rebuilt__v2022_08_11.tar falling-fluid-film-drl-rebuilt__v2022_08_11.tar__part.

To re-create the container you should do:

$ cat falling-fluid-film-drl-rebuilt__v2022_08_11.tar__part.?? > falling-fluid-film-drl-rebuilt__v2022_08_11.tar

Once the reconstruction of the container is done, you should check its hash to verify its integrity:

$ sha256sum falling-fluid-film-drl-rebuilt__v2022_08_11.tar 
d30eda25473dd5d219dabeca1f8e540d2b6bcbd293b54b3fba5ee393f7c15d10  falling-fluid-film-drl-rebuilt__v2022_08_11.tar

Using the container image

To use the container image:

• load the container image archive into docker

$ sudo docker image load < falling-fluid-film-drl-rebuilt__v2022_08_11.tar

• check that the image has well been loaded:

$ sudo docker image ls 
REPOSITORY                       TAG           IMAGE ID       CREATED         SIZE
falling-fluid-film-drl-rebuilt   v2022_08_11   751e15154f9d   4 minutes ago   2.48GB

• spin a new interactive container from the image, binding the TCP/UDP port:

~$ sudo docker run -it -p 8888:8888 falling-fluid-film-drl-rebuilt:v2022_08_11

• start a jupyter notebook inside the container:

root@2200b9f99d69:~# cd ~/drl-fluid-film-notebook/falling-liquid-film-drl/drl_fluid_film_python3/gym-film
root@2200b9f99d69:~/drl-fluid-film-notebook/falling-liquid-film-drl/drl_fluid_film_python3/gym-film# jupyter notebook --ip 0.0.0.0 --no-browser --allow-root

• open the link in your browser.

Following the "tutorials"

There is a small "tutorials" following the M1, M2, M3 methods reported in the paper: see the ipynb jupyter notebooks Introduction-and-method-M1.ipynb, Method-M2.ipynb, Method-M3.ipynb that should be visible in the jupyter file listing.

Copy paste of manual from https://github.com/vbelus/falling-liquid-film-drl

The paths are a bit messed up in the new image, and I recommend that you follow the jupyter notebooks to get understanding of the code, but reproducing some manual information for the sake of completeness:

The code is in drl_fluid_film_python3/gym-film. You find the following files:

• param.py contains the parameters that your next training will use (all the parameters of the project are centralized here)
• train.py is the script you will use to train or render a model

In gym_film, you will find the following directories:

• envs, where our basic environment class film_env.py is defined. It is a custom gym environment,and it interacts with the C++ simulation that is defined in simulation_solver.
• model, where the script to retrieve models is defined. These models are imported from the library stable_baselines, and only the PPO2 implementation has been used in the paper.
• results, where previously trained models are stored along with the parameters used for the training, and tensorboard logs to have insights on how the model performs during training

Execute the main script

The basic command is python3 train.py but you will need to add some flags :

• --train or -t to train your model
• --render or -r if you want to render the simulation

If you use this flag with -t, it will render during the training as well. You can change how often the rendering is done with the RENDER_PERIOD parameter

• --training_name or -tn is the name of the training, default value is "test"
• --load or -l followed by an integer n to load a trained model. This will look for a model trained for n episodes under the training name you specified
• --load_best or -lb will load the "best" model under the training name you specified, "best" meaning the model trained on k episodes, where the maximum episode reward of the entire training was obtained during episode k
• --port or -p, followed by an integer between 1024 and 49151, which will be the port used when using the multi-environment method (Method M3 in the paper).

If you want to train a model with the default parameters and render it, you can do it with python train.py --train --render --training_name my-first-training

Change the parameters of the training

All the parameters relevant to the training and simulation are in param.py. You will have to change the parameters in this file.

We will use the following syntax: parameter (type, typical low value - typical high value)

Some important parameters here are :

• The number of jets: n_jets (int, 1 - 20)
• The position of the jets: jets_position (array) OR position_first_jet (float) and space_between_jets (float, 5 - 20)
• The maximum power of the jets: JET_MAX_POWER (float, 1 - 15) and their width: JET_WIDTH (float, 2 - 10) -> As it is done, the action of the agent is always between -1 and 1 and is later normalized and multiplied by JET_MAX_POWER to be applied in the simulation. The default values are letting the jets modify q with the same amplitude as the waves naturally forming, so it should be enough for control.
• The size of the observation size_obs (float, 10 - 40), input of the agent, and the size of the observation on which the reward is calculated size_obs_to_reward (float, 5 - 20)
• The non-dimensional duration of one episode simulation_time (float, 5 - 20)
• The duration of the simulation before we begin any training initial_waiting_time (float). Default value is 200, letting the simulation get to a converged state before we do any training (the state is stored and not computed each time)
• simulation_step_time is the non-dimensional duration of one step of the simulation. In one such step, we do n_step steps of the numerical scheme
• Whether to render the simulation with matplotlib with render (bool). If True, render it every RENDER_PERIOD (int) environment steps

Video of the lecture at IFAIME

I was recently invited to give a guest lecture about DRL for flow control at IFAIME; the recording is available at: https://www.youtube.com/watch?v=SfbajZPvGoM .